Unveiling room temperature hydrogen storage in tubular graphitic carbon nitride with diverse morphologies

被引:2
作者
Guo, Ruiran [1 ]
Arkhurst, Barton [1 ]
Fan, Xinyue [1 ]
Lee, Min-wei [2 ]
Lin, Wen-jui [2 ]
Shih, Yung-Hsin [2 ]
Rokh, Ghazaleh Bahman [1 ]
Li, Honghao [1 ]
Sasmita, Sharon [1 ]
Zhou, Yifan [1 ]
Chan, Sammy Lap Ip [1 ,2 ]
机构
[1] Univ New South Wales, Sch Mat Sci & Engn, Sydney, NSW 2052, Australia
[2] Natl Cent Univ, Dept Chem & Mat Engn, Taoyuan 32001, Taiwan
关键词
Energy storage; Hydrogen adsorption/desorption; Surface area; COMPLEX HYDRIDES; ENERGY; NANOTUBES; PHOTOCATALYSIS; BEHAVIOR; ECONOMY;
D O I
10.1016/j.ecmx.2023.100496
中图分类号
O414.1 [热力学];
学科分类号
摘要
The 21st century stands as the hydrogen century, embodying profound possibilities for an economy driven by hydrogen. However, a main obstacle in realizing the hydrogen economy revolves around establishing a secure and efficient method for storing hydrogen. In this work, tubular graphitic carbon nitride (g-C3N4) was synthesized for the potential in hydrogen storage. The strategic fabrication of tubular g-C3N4 takes shape via three distinctive routes: hydrothermal, thermal condensation, and double calcination. Each pathway yields g-C3N4 with varying attributes such as surface area and size, thereby laying the groundwork for an intricate exploration and discussion of their hydrogen storage capabilities. Among the synthesized materials, those obtained through the hydrothermal route (H-g-C3N4) exhibited the most substantial dimensions, boasting an impressive length exceeding 10 mu m. Conversely, both the thermal condensation-derived nanotubes (T-g-C3N4) and their double calcination counterparts (D-g-C3N4) displayed similar dimensions, with lengths hovering around 1 mu m. It became evident that D-g-C3N4 exceeded the results of the other two samples in this aspect, showcasing an elevated BET surface area of 114.2 m2/g. In contrast, H-g-C3N4 and T-g-C3N4 demonstrated lower surface areas, registering at 59.3 and 70.2 m2/g. Regarding hydrogen storage, all samples were found to be able to adsorb and desorb hydrogen within 5 min. The hydrogen storage of the three distinct materials (H-g-C3N4, T-g-C3N4, and D-g-C3N4), as measured using a Sivert's system under room temperature and 3.7 MPa, manifested as 0.68 wt%, 0.72 wt%, and 0.8 wt%, respectively. This observed variation in storage capacity potentially found a correlation with the distinctive morphologies of the three materials. Despite the current hydrogen storage capacities of these materials being below 1 wt%, their inherent potential remains considerable. Achieving further advancements in fabrication techniques to enhance nanotube purity and reduce their size holds the promise of substantially augmenting their capacity for hydrogen storage.
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页数:7
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